Part of JME-10 — Thermal Properties: Expansion, Calorimetry & Heat Transfer

Apparent vs Real Expansion of Liquids

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When a liquid is heated in a container, both expand. What we observe (apparent expansion) is less than the actual (real expansion): γapparent=γrealγcontainer=γreal3αcontainer\gamma_{\text{apparent}} = \gamma_{\text{real}} - \gamma_{\text{container}} = \gamma_{\text{real}} - 3\alpha_{\text{container}}.

Mercury in glass: γHg=1.82×104\gamma_{\text{Hg}} = 1.82 \times 10^{-4} K1^{-1}, 3αglass2.7×1053\alpha_{\text{glass}} \approx 2.7 \times 10^{-5} K1^{-1}. Apparent expansion 1.55×104\approx 1.55 \times 10^{-4} K1^{-1}.

Overflow from a full flask: Voverflow=V0(γliquid3αcontainer)ΔTV_{\text{overflow}} = V_0(\gamma_{\text{liquid}} - 3\alpha_{\text{container}})\Delta T.

For accurate liquid expansion measurements, use fused quartz containers (α0.5×106\alpha \approx 0.5 \times 10^{-6}), minimizing the container correction. Mercury thermometers work on apparent expansion — the mercury in the glass tube rises because mercury expands more than glass.

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